PV – nbP- P"V" = 0 is found to be satisfied. When B and C are in thermal equilibrium the relation nB'P"V" P'V' – P"V" + V'

University Physics Volume 2
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Chapter2: The Kinetic Theory Of Gases
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Problem 34P: (a) What is the gauge pressure in a 25.0 cc car tire containing 3.60 mol of gas in a 30.0-L volume?...
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1. Systems A, B and C are gases with coordinates P, V ; P', V'; P",V" . When A and C are in
thermal equilibrium, the equation
PV – nbP- P"V" = 0
is found to be satisfied. When B and C are in thermal equilibrium the relation
nB'P"V"
P'V' – P"V" +:
V'
holds. The symbols n, b and B' are constants.
What are the three functions which are equal to each other at thermal equilibrium
and each of which is equal to 0, where Ois the empirical temperature.
b. What is the relation expressing the thermal equilibrium between A and B?
а.
Transcribed Image Text:1. Systems A, B and C are gases with coordinates P, V ; P', V'; P",V" . When A and C are in thermal equilibrium, the equation PV – nbP- P"V" = 0 is found to be satisfied. When B and C are in thermal equilibrium the relation nB'P"V" P'V' – P"V" +: V' holds. The symbols n, b and B' are constants. What are the three functions which are equal to each other at thermal equilibrium and each of which is equal to 0, where Ois the empirical temperature. b. What is the relation expressing the thermal equilibrium between A and B? а.
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